Phonostat: Thermostatting phonons in molecular dynamics simulations

Thermostat algorithms in a molecular dynamics simulation maintain an average temperature of a system by regulating the atomic velocities rather than the internal degrees of freedom. Herein, we present a "phonostat" algorithm that can regulate the total energy in a given internal degree of...

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Bibliographic Details
Main Authors: Raghunathan, Rajamani (Contributor), Greaney, P. Alex (Contributor), Grossman, Jeffrey C. (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Materials Science and Engineering (Contributor)
Format: Article
Language:English
Published: American Institute of Physics (AIP), 2013-07-22T18:48:39Z.
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Online Access:Get fulltext
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100 1 0 |a Raghunathan, Rajamani  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Materials Science and Engineering  |e contributor 
100 1 0 |a Raghunathan, Rajamani  |e contributor 
100 1 0 |a Greaney, P. Alex  |e contributor 
100 1 0 |a Grossman, Jeffrey C.  |e contributor 
700 1 0 |a Greaney, P. Alex  |e author 
700 1 0 |a Grossman, Jeffrey C.  |e author 
245 0 0 |a Phonostat: Thermostatting phonons in molecular dynamics simulations 
260 |b American Institute of Physics (AIP),   |c 2013-07-22T18:48:39Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/79661 
520 |a Thermostat algorithms in a molecular dynamics simulation maintain an average temperature of a system by regulating the atomic velocities rather than the internal degrees of freedom. Herein, we present a "phonostat" algorithm that can regulate the total energy in a given internal degree of freedom. In this algorithm, the modal energies are computed at each time step using a mode-tracking scheme and then the system is driven by an external driving force of desired frequency and amplitude. The rate and amount of energy exchange between the phonostat and the system is controlled by two distinct damping parameters. Two different schemes for controlling the external driving force amplitude are also presented. In order to test our algorithm, the method is applied initially to a simple anharmonic oscillator for which the role of various phonostat parameters can be carefully tested. We then apply the phonostat to a more realistic (10,0) carbon nanotube system and show how such an approach can be used to regulate energy of highly anharmonic modes. 
520 |a United States. Defense Threat Reduction Agency (United States. Dept. of Defense. Joint Science and Technology Office for Chemical and Biological Defense Grant HDTRA1-09-1-0006) 
546 |a en_US 
655 7 |a Article 
773 |t The Journal of Chemical Physics